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2021ApJ...910...30T - Astrophys. J., 910, 30-30 (2021/March-3)

Merger rate density of Population III binary black holes below, above, and in the pair-instability mass gap.

TANIKAWA A., SUSA H., YOSHIDA T., TRANI A.A. and KINUGAWA T.

Abstract (from CDS):

We present the merger rate density of Population III binary black holes (BHs) by means of a widely used binary population synthesis code BSE with extensions to very massive and extreme metal-poor stars. We consider not only low-mass BHs (lBHs: 5-50M☉) but also high-mass BHs (hBHs: 130-200M☉), where lBHs and hBHs are below and above the pair-instability mass gap (50-130M☉), respectively. Population III BH-BHs can be categorized into three subpopulations: BH-BHs without hBHs (hBH0s: mtot <= 100M☉), with one hBH (hBH1s: mtot ∼ 130-260M☉), and with two hBHs (hBH2s: mtot ∼ 270-400M☉), where mtot is the total mass of a BH-BH. Their merger rate densities at the current universe are ∼0.1 yr–1 Gpc–3 for hBH0s, and ∼0.01 yr–1 Gpc–3 for the sum of hBH1s and hBH2s, provided that the mass density of Population III stars is ∼1013M☉ Gpc–3. These rates are modestly insensitive to initial conditions and single star models. The hBH1 and hBH2 mergers can dominate BH-BHs with hBHs discovered in the near future. They have low effective spins <=0.2 in the current universe. The number ratio of hBH2s to hBH1s is high, >=0.1. We also find that BHs in the mass gap (up to ∼85M☉) merge. These merger rates can be reduced to nearly zero if Population III binaries are always wide (>=100R☉), and if Population III stars always enter into chemically homogeneous evolution. The presence of close Population III binaries (∼10R☉) is crucial for avoiding the worst scenario.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Astrophysical black holes - Stellar mass black holes - Massive stars - Close binary stars - Common envelope binary stars - Population III stars - Gravitational waves

Simbad objects: 3

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